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Introduction
Optimization of a building structure is a complicated task. The steel
skeletal structures in tall buildings are very complicated systems
that must never fail. These structures can usually be broken down
into a system of columns, beams, and wind bracings, all of which can
be modeled as simple beam and truss structures. With the increasing
popularity and computing power of computers, the place for computers
in design is greater than ever, especially in optimization. But when
is a design optimal? Is an optimized design strictly the one that
uses the least material and is sufficiently strong? Civil Engineers
often look at the beauty of a design by how well it parallels nature,
which tends to create efficient and symmetrical designs. On the other
hand, if all designs were optimized toward one scheme, virtually all
bridges and buildings would look the same. Architects tend to focus
more on the aesthetic design of a structure. Asymmetry can be
intriguing and striking, while innovative truss designs can add
character as well as a sound structural basis for a building. This
report examines three computational methods of optimization of
building structures, two of which allow for unique but still optimal
designs to be generated.
Most
optimization schemes for building structures can be broken down into
two parts, the mathematical relations that solve for the desired
parameter to be optimized (ie. stress), and the numerical methods used
to search the problem space for the optimum solution. The methods
discussed in this report fall into this latter category.
Nevertheless, a brief discussion of the mathematics behind this
analysis will be discussed here.
Analysis of a computer model is governed by mathematical and physical
laws. These mathematical relations provide the foundation of
virtually all computational structural optimization algorithms. A
common method for determining stresses, forces, and displacements, is
to use a similar method to using Kirchoff’s node law and Ohm’s law to
solve for electrical currents and voltages. This method also models
the beams and trusses of a structure as a network of one-dimensional
elements with the primary difference being that the forces and
displacements are vectors instead of the scalar quantities used when
analyzing voltages and currents as seen in the figure below where (b)
is the electrical analog of a structural problem (a). Applying this
concept further by shrinking these beams and trusses down to very
large but finite arrays of small sized elements allows for analysis of
complex geometries. This method is better known as the finite element
method, and is how almost all stresses and strains are determined
computationally. The stress analysis criteria of all of the
structural optimization methods discussed in this report are also
based on this finite element method. [6]

By
using these mathematical relations and searching the design space of
potential outcomes based on varying each parameter, optimal designs
can be found. The methodology of searching this design space is the
focus of the rest of this report.
Click here to continue to the Overview of
Methods section.
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